RIAA Preamps Part 2 - Tube CAD Journal
RIAA Preamps Part 2 - Tube CAD Journal
RIAA Preamps Part 2 - Tube CAD Journal
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+210V<br />
5.5k<br />
8k<br />
11k<br />
+100V<br />
.0099µF<br />
+130V<br />
117k<br />
+130V<br />
.47µF<br />
300 32.5k<br />
6DJ8 +2V 6DJ8 +2V<br />
300<br />
.03µF<br />
6DJ8 +24V<br />
.1µF 300<br />
6DJ8 +2V<br />
1M<br />
47k<br />
200<br />
200<br />
8.7k<br />
24k<br />
1M<br />
200<br />
Cascading these two functions results in the<br />
same curve as the traditional two function<br />
combination creates. So, why bother with this<br />
alternate approach Beyond the mental<br />
stretching, which is always for the good, this<br />
alternative approach engenders new phono<br />
preamp topologies, with some interesting<br />
benefits and one negative. The first benefit is<br />
that the 50Hz low-pass filter can filter more<br />
power supply noise away from the output signal<br />
than the 2122Hz can.<br />
.1µF<br />
1M<br />
+10V<br />
200<br />
47k<br />
Ra<br />
1200<br />
10k<br />
91k<br />
R1<br />
C1<br />
+12V<br />
C2<br />
Rk<br />
.266µF<br />
+210V<br />
.0318µF<br />
A single-triode phono preamp<br />
Second, the 500Hz to 2122Hz shelving<br />
network can be implemented within one<br />
grounded–cathode amplifier, i.e. a single triode<br />
<strong>RIAA</strong> equalized preamp. Usually a cathode<br />
resistor is bypassed with a large valued<br />
capacitor, so as to ensure adequate lowfrequency<br />
response. But if the bypass capacitor’s<br />
value is reduced greatly, it introduces a shelving<br />
function, wherein the high-frequency gain is<br />
greater than the low-frequency gain, with the<br />
ratio being equal to the bypassed gain over the<br />
unbypassed gain or<br />
1 .<br />
Ratio = 1 + (mu + 1)R k<br />
R a + r p<br />
The transition frequencies are based on the<br />
capacitor’s value and the time constants it forms<br />
with the triode’s r p and its plate and cathode<br />
resistor values:<br />
R k C k = 75µS<br />
[(R a + r p )/(mu + 1) || R k ]C k = 318µS<br />
Of course, one triode is not going to provide<br />
enough gain in most cases, so additional gain<br />
stages will be needed.<br />
The overarching liability of this different<br />
path to <strong>RIAA</strong> equalization is the –12dB insertion<br />
loss beyond the expected losses, which brings it<br />
1kHz insertion loss down to –32dB. With this<br />
equalization network, the near DC and subsonic<br />
frequencies are reduced by –12dB, whereas the<br />
traditional path retained all of the gain at the<br />
bottom of range. Now, -12dB is just too much to<br />
pay in most two-gain-stage phono preamps, but<br />
it is almost nothing in a three-gain-stage preamp,<br />
where the problem is usually having too much<br />
gain. Still the advantage of using a portion of the<br />
equalization network in double duty either, as a<br />
pseudo coupling capacitor or a partial cathodebypass<br />
capacitor, is tempting.<br />
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